Classical thermodynamics: Difference between revisions
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*[[Gibbs-Helmholtz equations]] | *[[Gibbs-Helmholtz equations]] | ||
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*[[Gibbs phase rule]] | |||
*[[Griffiths phase rule]] | |||
==H== | ==H== | ||
*[[Heat]] | *[[Heat]] |
Revision as of 14:19, 10 December 2009
- "...all the signs suggest that the main principles of thermodynamics from the classical theory will not only rule unchallenged but will more probably become correspondingly extended."
- Max Planck "The Genesis and Present State of Development of the Quantum Theory" Nobel Lecture, June 2, 1920
- "...the deep impression that classical thermodynamics made upon me. It is the only physical theory of universal content concerning which I am convinced that, within the framework of the applicability of its basic concepts, it will never be overthrown."
- Albert Einstein "Autobiographical Notes"
B
C
- Capillary waves
- Carnot cycle
- Charles's law
- Chemical potential
- Clausius-Clapeyron relation
- Clausius theorem
- Compressibility
- Compressibility factor
- Critical points
D
E
F
G
- Gay-Lussac's law
- Gibbs-Duhem relation
- Gibbs-Helmholtz equations
- Gibbs energy function
- Gibbs phase rule
- Griffiths phase rule
H
I
J
L
M
P
R
S
T
- Temperature
- Thermal expansion coefficient
- Thermodynamic integration
- Thermodynamic potential
- Thermodynamic relations
- Third law of thermodynamics
- Triple point